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Fast Calcium Transients in Neuronal Spines Driven by Extreme Statistics bioRxiv preprint doi: https://doi.org/10.1101/290734; this version posted April 8, 2018. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. Fast calcium transients in neuronal spines driven by extreme statistics Kanishka Basnayakea, Eduard Korkotianb, and David Holcmana aComputational Biology and Applied Mathematics, École Normale Supérieure, Paris 75005, France. bNeurobiology, Weizmann Institute of Science, Rehovot 76100, Israel. April 5, 2018 Keywords: Calcium transients; Endoplasmic Reticulum; Diusion; Extreme statistics; First Passage Times; Biophysical Modeling; Dendritic Spines Abstract Fast calcium transients (< 10ms) remain dicult to analyse in cellular mi- crodomains, yet they can modulate key cellular events such as tracking, local ATP production by ER-mitochondria complex or spontaneous activity in astrocytes. In dendritic spines receiving synaptic inputs, we show here that in the presence of a spine apparatus (SA), which is an extension of the smooth ER, a calcium-induced calcium release is triggered at the base of the spine by the fastest calcium ions arriv- ing at a Ryanodine receptor. The mechanism relies on the asymmetric distributions of Ryanodine receptors and SERCA pumps that we predict using a computational model and further conrm experimentally. The present mechanism where the statis- tics of the fastest particles arriving at a small target followed by an amplication is likely to be generic in molecular transduction across cellular micro-compartments such as astrocytes, endfeets and protrusions. 1 Introduction Extreme statistics describes the distribution of rare events such as the rst ions to nd a small target [1,2], which are dicult to detect experimentally in biological microdomains. However, indirect signatures can be derived from their statistical properties. We examine here the role of rare events associated to calcium dynamics in dendritic spines, that are 1 bioRxiv preprint doi: https://doi.org/10.1101/290734; this version posted April 8, 2018. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. local microdomains located on the dendrites of neuronal cells. Spines can form synap- tic connections that transmit neural activity [3, 4]. Here we describe specically how the fastest calcium ions dene the time scale of calcium transduction when it is followed by an amplication step. Regulating this fast event has many consequences in the induction of plastic changes. Indeed, calcium increase can be restricted to the spine head isolated from the dendrite, enabling the induction of local synapse-specic calcium-dependent plasticity leading to AMPA receptor accumulations [5, 6]. A fast and localized amount of calcium ions is necessary to induce ATP production from mitochondria to supply the energy re- quired to maintain homeostasis [79]. Spines are characterized by the diversity of their shapes, sizes, and the presence or ab- sence of dierent structural components and organelles such as an endoplasmic reticu- lum. During synaptic plasticity, spine morphology [1012] can change, leading to an increase/decrease of the head size [13] or an elongation/retraction of their neck. Neck elongation can further lead to electrical and biochemical isolation from their parent den- drites [1420]. Spines can contain a smooth endoplasmic reticulum (ER), fragmented in a compartment called the spine apparatus (SA), that can regulate calcium ions by storing or releasing them [21,22] and modulate synaptic inputs [23,24]. The SA is monitored by the actin-associated protein synaptopodin (SP) that can modulate calcium kinetics [2527]. After calcium ions enter into dendritic spines, they can bind to endogeneous buers, get extruded by pumps into the extracellular medium or be pumped into the SA by the sarco/endoplasmic reticulum calcium-ATPase pumps (SERCA3). Calcium ions can also induce calcium release from internal SA stores through the ryanodine receptors (RyR) [22,28]. However, the specic calcium regulation by SA remains unclear due to the fast dynamics and the spine's nanometer-scale organization. We recall that the time scale of calcium diusion transient during long-term plasticity [29] is of the order of hundreds of milliseconds [3,30] but not faster. We show here that the mechanism involved in fast calcium transient (faster than tens of milliseconds) relies on a new mechanism associated to the extreme statistics of the fastest ions that we describe here. For that purpose, we develop a computational model for cal- cium ion dynamics and use stochastic simulations to interpret uncaging and uorescent imaging. To simulate calcium dynamics in synapses and dendritic spines, there are two possible approaches: deterministic reaction-diusion equations [31,32] or stochastic mod- eling [3337] that we use here. With this approach, we obtain a new understanding of fast calcium transients. Indeed, after calcium ions are released inside the spine head using ash photolysis of caged calcium, the concentration increase at the dendrite is faster in spines containing a SA compared to those where it is absent. This is a paradox as the SA should obstruct the passage from the spine head to the dendrite and prevent calcium ions from diusing. To address this paradox, we use stochastic simulations to show that after calcium released in the spine head, the fastest ions arriving at the base determine the timescale of calcium transient due to an amplication step. Furthermore, we nd that the distribution of arrival times of the fastest ions depends on the initial number of calcium ions, which is a signature of extreme statistics and rare events. Finally, we 2 bioRxiv preprint doi: https://doi.org/10.1101/290734; this version posted April 8, 2018. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. suggest that molecular activation initiated by the fastest particles is a generic mechanism in molecular transduction that can occurs in cellular micro-compartments such as protru- sions, astrocytic endfeets and more. This mechanism is likely to dene the timescale of biochemical activation in nano- and micro-domains, when the source of diusing particles and the binding targets are spatially separated. Methods Stochastic simulations of calcium ions in a dendritic spine We model a dendritic spine with a spherical head connected to a narrow, cylindrical neck [35] (Fig. 1A). The SA is also modeled with a similar geometry with a neck and a head positioned inside the spine (Fig. 2G). Calcium ions are describedp as Brownian particles following the Smoluchowski limit of the Langevin equation X_ = 2Dw_ , where w is the Wiener white noise. This motion of particles is simulated using the Euler's scheme. Ions can diuse inside the cytoplasm, and they are reected at the surfaces of the spine and the SA (Snell-Descartes reection). To replicate the uncaging experiments, we use either the center of the ball or the base of the cylindrical neck as the initial positions of particles. Ions arriving at the dendritic shaft located at the base are considered to be lost and do not return to the spine during the timescale of the simulations (absorbing boundary). The inner surface of the spine head contains 50 absorbing circular disks with a 10nm radius, which models calcium pumps. Ryanodine receptors RyRs are activated upon the arrival of the rst two ions [38] to a small absorbing disk of size aRyR = 10nm (see SI for further descriptions). We positioned nR = 36 receptors for the simulations organized in four rings in the SA neck, each containing six receptors. The other 12 are located on the SA component parallel to the dendritic shaft (see gure legends). After a receptor opens, it releases instantaneously a xed number of calcium ions nCa, which are positioned at the center of the receptors. Following this release, the RyR enters into a refractory period that lasts 3 to 6ms, during which it is modeled as a reective boundary. In Fig 4B, we nd that calcium ions should be released with a delay of 0.25ms after the arrival of a second ion to the RyR binding site. SERCA pumps We positioned 36 SERCA pumps uniformly distributed on the upper hemisphere of the spine head. They are modeled as absorbing disks of size aSERCA = 10nm. When a calcium ion arrives to the disk, it is bound indenitely. If a second ion arrives, both are absorbed immediately and the transporter is frozen in an inactive state. 3 bioRxiv preprint doi: https://doi.org/10.1101/290734; this version posted April 8, 2018. The copyright holder for this preprint (which was not certified by peer review) is the author/funder. All rights reserved. No reuse allowed without permission. Mean rst passage time of ions to the base of a spine For a Brownian particle released in the spine head, the mean arrival time to the base of a spine has been computed asymptotically [37] V a R L2 V L τ¯ = [1 + log( )] + + ; (1) 4Da πR a 2D πDa2 where D is the diusion coecient, a, R and L are the spine neck radius, head radius and the total length of the neck respectively. We refer to Table 1 (SI) for the parameter values, from which we estimated τ¯ ≈ 120ms. Experimental procedure Cultured hippocampal neurons were transfected with DsRed and loaded with NP-EGTA AM (caged calcium buer) after which several specic cells were microinjected with Fluo-4 calcium sensor. UV laser was directed to either spine heads or the basal dendritic shafts. Following the ashes of ND-YAG UV laser (4 ns, 330 nm) focused into a region of about 0.5 µm in diameter, the released calcium signals could be detected and line-scanned using confocal microscope at the rate of 0.7 ms/line.
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